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If you take the model in Ex. 4.1 at face value, what natural frequency do you get? Put in the actual numbers. Where, in the electromagnetic spectrum, does this lie, assuming the radius of the atom is 0.5 Å? Find the coefficients of refraction and dispersion, and compare them with the measured values for hydrogen at 0°Cand atmospheric pressure:A=1.36×10-4,B=7.7×10-15m2 .

Short Answer

Expert verified

The natural frequency is 7.16×1015 Hz, and it lies in ultraviolet range. The coefficient of refraction is4.2×105 , and it is about13 of the actual value. The coefficient of dispersionis 1.8×1015 m2, and it is about 14of the actual value.

Step by step solution

01

Expression forthe electric field, and binding force: 

Write the expression forelectric field.

E=14πε0qda3 …… (1)

Here, ε0is the permittivity of free space, q is the charge, d is the distance and a is the radius of an atom.

Write the expression for binding force using equation (1) as,

Fbinding=-qE=-(14πε0q2a3)x=-kspringx …… (2)

Here,kspring is the spring constant.

02

Determine the natural frequency:

Substitute Fbinding=14πε0q2a3and kspring=mω02in equation (2).

(14πε0q2a3)x=mω02xω0=q24πε0ma3 …… (3)

Write the expression for the natural frequency.

ν0=ω02π

Substituteω0=q24πε0ma3 in the above expression.

ν0=12πq24πε0ma3 …… (4)

Here, qis charge of electron,m is mass of electron, ε0is permittivity of space, anda is distance.

Substitute ,q=1.6×1019 C ,ε0=8.85×1012 C2/Nm2,m=9.11×1031 kgand a=0.5A0in equation (4).

ν0=12π(1.6×1019 C)24π(8.85×1012 C2/Nm2)(9.11×1031 kg)(0.5A0×1010 m1A0)3ν0=7.16×1015 Hz

Therefore, the natural frequency is 7.16×1015 Hz, and it lies in ultraviolet range.

03

Determine the expression for coefficient of refraction (A) and coefficient of dispersion (B): 

Write the formula for the index of refraction.

n=1+(Nq22mε0jfjωj2)+ω2(Nq22mε0jfjωj4)n=1+A(1+Bλ2)

Here,λ is the wavelength.

Here,λ=2πcω0

Write the formula for coefficient of refraction (A).

A=Nq22mε0fω02 …… (5)

Here, Nis number of molecules per unit volume, and fnumber of electrons per molecules.

Here,f=2(for H2) .

Write the formula for coefficient of dispersion (B).

B=(2πcω0)2 …… (6)

Here, c is the speed of light.

04

Determine the coefficient of refraction (A) and coefficient of dispersion (B):

Substituteq=1.6×1019 C,ε0=8.85×1012 C2/Nm2, m=9.11×1031 kgand a=0.5A0in equation (3).

ω0=q24πε0ma3ω0=(1.6×1019 C)24π(8.85×1012)(9.11×1031 kg)(0.5A0×1010 m1A0)3ω0=4.5×1016 Hz

Calculate the value of Nas follows.

N=Avogadro’s number22.4 LN=6.02×102322.4×103N=2.69×1025

SubstituteN=2.69×1025, q=1.6×1019 C,f=2,m=9.11×1031 kg, ε0=8.85×1012 C2/Nm2andω0=4.5×1016 Hzin equation (5).

A=(2.69×1025)(1.6×1019 C)2(2)2(9.11×1031 kg)(8.85×1012 C2/Nm2)(ω0=4.5×1016 Hz)2A=4.2×105

This value is about13of the actual value.

Substitutec=3×108 m/sandω0=4.5×1016 Hzin equation (6).

B=(2π×3×1084.5×1016)2B=1.8×1015 m2

This value is about 14of the actual value.

Therefore, the coefficient of refraction is 4.2×105and it is about 13of the actual value. The coefficient of dispersionis 1.8×1015 m2, and it is about14 of the actual value.

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Most popular questions from this chapter

Calculate the reflection coefficient for light at an air-to-silver interface (μ1=μ2=μ0,ε=ε0,σ=6×107(Ωm)-1)at optical frequencies(ω=4×1015/s).

Light from an aquarium goes from water (n=43)through a plane of glass (n=32)into the air (n=1). Assuming its a monochromatic plane wave and that it strikes the glass at normal incidence, find the minimum and maximum transmission coefficients (Eq. 9.199). You can see the fish clearly; how well can it see you?

SupposeAeiax+Beibx=Ceicx, for some nonzero constants A, B, C, a, b, c, and for all x. Prove that a = b = cand A + B = C.

Question:According to Snell's law, when light passes from an optically dense medium into a less dense one the propagation vector bends away from the normal (Fig. 9.28). In particular, if the light is incident at the critical angle

θc=sin-(n2n1)

Then , and the transmitted ray just grazes the surface. If exceeds , there is no refracted ray at all, only a reflected one (this is the phenomenon of total internal reflection, on which light pipes and fiber optics are based). But the fields are not zero in medium ; what we get is a so-called evanescent wave, which is rapidly attenuated and transports no energy into medium 2.26

Figure 9.28

A quick way to construct the evanescent wave is simply to quote the results of Sect. 9.3.3, with and

kT=kTsinθTx^+cosθTz^

the only change is that

sinθT=n1n2sinθI

is now greater than, and

cosθT=1-sin2θT

is imaginary. (Obviously, can no longer be interpreted as an angle!)

(a) Show that

ET(r,t)=E0Te-kzeI(kx-ωt)

Where

kωc(n1sinθ1)2-n22

This is a wave propagating in the direction (parallel to the interface!), and attenuated in the direction.

(b) Noting that (Eq. 9.108) is now imaginary, use Eq. 9.109 to calculate theirreflection coefficient for polarization parallel to the plane of incidence. [Notice that you get reflection, which is better than at a conducting surface (see, for example, Prob. 9.22).]

(c) Do the same for polarization perpendicular to the plane of incidence (use the results of Prob. 9.17).

(d) In the case of polarization perpendicular to the plane of incidence, show that the (real) evanescent fields are

Er,t=E0e-kzcoskx-ωty^Br,t=E0ωe-kzksinkx-ωtx^+kcoskx-ωtz^

(e) Check that the fields in (d) satisfy all of Maxwell's equations (Eq. 9.67).

(f) For the fields in (d), construct the Poynting vector, and show that, on average, no energy is transmitted in the z direction.

Question: Show that the standing wave fz,t=Asinkzcoskvtsatisfies the wave equation, and express it as the sum of a wave traveling to the left and a wave traveling to the right (Eq. 9.6).

See all solutions

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